Dynamics September 6-4 1708.07400.Pdf

Dynamics of Current, Charge and Mass Bob Eisenberg Department of Applied Mathematics Illinois Institute of Technology USA Department of Physiology and Biophysics Rush University USA [email protected] Xavier Oriols Departament d’Enginyeria Electrònica, Universitat Autònoma de Barcelona, SPAIN [email protected] David Ferry School of Electrical, Computer, and Energy Engineering Arizona State University USA [email protected] Available on arXivhttps://arxiv.org/abs/1708.07400 at September 6, 2017 ABSTRACT Electricity plays a special role in our lives and life. The dynamics of electrons allow light to flow through a vacuum. The equations of electron dynamics are nearly exact and apply from nuclear particles to stars. These Maxwell equations include a special term, the displacement current (of a vacuum). The displacement current allows electrical signals to propagate through space. Displacement current guarantees that current is exactly conserved from inside atoms to between stars, as long as current is defined as the entire source of the curl of the magnetic field, as Maxwell did. We show that the Bohm formulation of quantum mechanics allows the easy definition of current without the mysteries of the theory of quantum measurements. We show how conservation of current can be derived without mention of the polarization or dielectric properties of matter. We point out that displacement current is handled correctly in electrical engineering by ‘stray capacitances’, although it is rarely discussed explicitly. Matter does not behave as physicists of the 1800's thought it did. They could only measure on a time scale of seconds and tried to explain dielectric properties and polarization with a single dielectric constant, a real positive number independent of everything. Matter and thus charge moves in enormously complicated ways that cannot be described by a single dielectric constant, when studied on time scales important today for electronic technology and molecular biology. When classical theories could not explain complex charge movements, constants in equations were allowed to vary in solutions of those equations, in a way not justified by mathematics, with predictable consequences. Life occurs in ionic solutions where charge is moved by forces not mentioned or described in the Maxwell equations, like convection and diffusion. These movements and forces produce crucial currents that cannot be described as classical conduction or classical polarization. Derivations of conservation of current involve oversimplified treatments of dielectrics and polarization in nearly every textbook. Because real dielectrics do not behave in that simple way—not even approximately—classical derivations of conservation of current are often distrusted or even ignored. We show that current is conserved inside atoms. We show that current is conserved exactly in any material no matter how complex are the properties of dielectric, polarization, or conduction currents. Electricity has a special role because conservation of current is a universal law. Most models of chemical reactions do not conserve current and need to be changed to do so. On the macroscopic scale of life, conservation of current necessarily links far spread boundaries to each other, correlating inputs and outputs, and thereby creating devices. We suspect that correlations created by displacement current link all scales and allow atoms to control the machines and organisms of life. Conservation of current has a special role in our lives and life, as well as in physics. We believe models, simulations, and computations should conserve current on all scales, as accurately as possible, because physics conserves current that way. We believe models will be much more successful if they conserve current at every level of resolution, the way physics does. We surely need successful models as we try to control macroscopic functions by atomic interventions, in technology, life, and medicine. Maxwell’s displacement current lets us see stars. We hope it will help us see how atoms control life. 1 September 6, 2017 https://arxiv.org/abs/1708.07400 1. INTRODUCTION The dynamics of electrons allow us to hold a computer in our hand that detects signals of microvolts, from a 500 watt satellite source some 22,200 miles away. The computer in our hand makes logical decisions nearly a billion times a second, using some 1012 components, with hardly any errors. The fundamental laws that govern these phenomena are Maxwell’s equations. These laws are so general that they are often thought to have limited practical applicability: their application is often thought to depend on precise knowledge of the detailed properties of matter, knowledge that is often unknown, always hard to acquire. This paper is about a notable exception: conservation of current. Conservation of current is true universally, on all scales, independent of the detailed properties of matter. Kirchhoff’s current law illustrates the importance of conservation of current. Kirchoff’s laws use a set of currents and voltages to predict the performance of systems operating with currents ranging from femtoamps to kiloamps, with potentials from microvolts to hundreds of volts, in resistors ranging from tenths of an ohm to sometimes tens of gigohms. Kirchoff’s laws are simple, compact and easy to use. They are also exact in branched one dimensional systems, when current is defined to include displacement current. Electrical systems follow Kirchoff’s current law exactly because conservation of current is universal. Electricity is Different because few physical systems follow simple and compact laws with such precision. Electricity is familiar as well as different because it is used so widely in our technology and life. Our society of information (with its internet of everything) is a practical application of the dynamics of electrons. Our technology would be impossible if Kirchoff’s laws were not accurate and easy to apply. Electricity is so widely used because it follows universal laws that can be easily applied. Compact and simple laws, like Kirchhoff’s laws, allow the use of mathematics to design devices with a wide range of properties (Gray, Hurst et al. 2001, Cressler 2005, Horowitz and Hill 2015) with reasonable realism. For example, the microchip in your laptop computer requires manufacturing precision to sub-nanometer accuracy across 300 millimeters of the semiconductor wafer in which the computer chip is formed. This accuracy is an incredible feat of today’s technology. Sciences that depend on less accurate, simple and compact laws are often forced to use models that are not ‘transferrable’ (as the word is used by chemists). We mean by ‘transferable’ that the same law—with the same numerical value of parameters—can be used in a multitude of conditions and systems and is not constrained to a single system and set of conditions. Non-transferrable models use parameters that change with conditions, often in ways that are hard to capture or predict. Devices become difficult to use when their parameters and properties vary in unpredictable ways. Nearly all systems — particularly liquids and ionic solutions so important in chemistry and biology — involve many types of forces and interactions. Interacting systems are particularly difficult to capture in simple and compact laws. Interactions make it difficult to find transferrable models, with one set of unchanging parameters valid for a 2 September 6, 2017 https://arxiv.org/abs/1708.07400 large range of conditions. The simple and compact transferable models valid for typical electronic technology cannot be automatically applied to biological systems because of their complex structure, but the electrical properties of individual nerve and muscle fibers can be expressed in terms of Kirchoff’s laws and little else, amazingly enough. (Hodgkin and Huxley 1952c, Hodgkin 1958, Hodgkin 1964, Hodgkin 1992, Weiss 1996, Huxley 2000, Huxley 2002, Prosser, Curtis et al. 2009, Gabbiani and Cox 2010). Even electrical syncytia like the heart, epithelia, lens of the eye, liver, and so on can be described quite well with modest generalizations of Kirchoff’s laws.(Tung 1978, Eisenberg, Barcilon et al. 1979, Mathias, Rae et al. 1979, Eisenberg and Mathias 1980, Mathias, Rae et al. 1981, Geselowitz and Miller 1983, Levis, Mathias et al. 1983) Nerve and muscle fibers live in salt solutions derived from seawater, as does nearly all of life. Many chemical systems and a great deal of our chemical technology involve these salt solutions. Interactions abound in salt solutions, and they occur between the different types of ions, and ions with the water. Seawater flows in pressure and temperature gradients, so many types of forces are involved. Electric fields are particularly important in these systems and they pose particular problems because electric fields are very strong and extend a very long way, coupling atomic and macroscopic length scales with one set of physical laws. Viewed physically, most biological systems of interest are macroscopic systems containing a huge number of fundamental particles with a fantastic number of interactions between pairs of particles. The number of interactions is orders of magnitude larger than Avogadro’s number or 1023 for the number of particles per mole. Even small systems contain millions of molecules, and larger systems contain 1017 molecules, pairwise interactions can dominate properties. The attempts to describe the system by computing the dynamics of each particle becomes, in general,

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